Jump to
S1C2
Energy calculated at PBEPBE/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -134.993372 |
| Energy at 298.15K | -135.001457 |
| Nuclear repulsion energy | 82.277443 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Vibrational Frequencies calculated at PBEPBE/6-31G(2df,p)
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A' |
3385 |
3350 |
2.38 |
|
|
|
| 2 |
A' |
3040 |
3009 |
38.51 |
|
|
|
| 3 |
A' |
2965 |
2934 |
39.68 |
|
|
|
| 4 |
A' |
2960 |
2930 |
18.80 |
|
|
|
| 5 |
A' |
1618 |
1601 |
15.01 |
|
|
|
| 6 |
A' |
1454 |
1439 |
1.32 |
|
|
|
| 7 |
A' |
1434 |
1419 |
0.02 |
|
|
|
| 8 |
A' |
1353 |
1339 |
6.04 |
|
|
|
| 9 |
A' |
1331 |
1317 |
14.14 |
|
|
|
| 10 |
A' |
1133 |
1121 |
8.19 |
|
|
|
| 11 |
A' |
1042 |
1031 |
21.93 |
|
|
|
| 12 |
A' |
886 |
877 |
90.34 |
|
|
|
| 13 |
A' |
849 |
841 |
65.46 |
|
|
|
| 14 |
A' |
387 |
383 |
4.97 |
|
|
|
| 15 |
A" |
3464 |
3428 |
0.44 |
|
|
|
| 16 |
A" |
3044 |
3012 |
45.51 |
|
|
|
| 17 |
A" |
3000 |
2969 |
10.06 |
|
|
|
| 18 |
A" |
1446 |
1431 |
6.29 |
|
|
|
| 19 |
A" |
1356 |
1342 |
0.01 |
|
|
|
| 20 |
A" |
1232 |
1220 |
0.04 |
|
|
|
| 21 |
A" |
980 |
970 |
1.15 |
|
|
|
| 22 |
A" |
754 |
746 |
1.68 |
|
|
|
| 23 |
A" |
292 |
289 |
33.90 |
|
|
|
| 24 |
A" |
250 |
247 |
9.37 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 19826.7 cm
-1
Scaled (by 0.9897) Zero Point Vibrational Energy (zpe) 19622.5 cm
-1
See section
III.C.1 List or set vibrational scaling factors
to change the scale factors used here.
See section
III.C.2
Calculate a vibrational scaling factor for a given set of molecules
to determine the least squares best scaling factor.
Geometric Data calculated at PBEPBE/6-31G(2df,p)
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
-1.318 |
-0.075 |
0.000 |
| C2 |
0.000 |
0.575 |
0.000 |
| C3 |
1.216 |
-0.362 |
0.000 |
| H4 |
2.165 |
0.201 |
0.000 |
| H5 |
1.212 |
-1.014 |
0.891 |
| H6 |
1.212 |
-1.014 |
-0.891 |
| H7 |
0.044 |
1.240 |
-0.882 |
| H8 |
0.044 |
1.240 |
0.882 |
| H9 |
-1.374 |
-0.700 |
0.812 |
| H10 |
-1.374 |
-0.700 |
-0.812 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
C3 |
H4 |
H5 |
H6 |
H7 |
H8 |
H9 |
H10 |
| N1 | | 1.4700 | 2.5506 | 3.4946 | 2.8420 | 2.8420 | 2.0891 | 2.0891 | 1.0258 | 1.0258 |
C2 | 1.4700 | | 1.5354 | 2.1975 | 2.1881 | 2.1881 | 1.1052 | 1.1052 | 2.0426 | 2.0426 | C3 | 2.5506 | 1.5354 | | 1.1037 | 1.1039 | 1.1039 | 2.1718 | 2.1718 | 2.7352 | 2.7352 | H4 | 3.4946 | 2.1975 | 1.1037 | | 1.7829 | 1.7829 | 2.5210 | 2.5210 | 3.7413 | 3.7413 | H5 | 2.8420 | 2.1881 | 1.1039 | 1.7829 | | 1.7816 | 3.0960 | 2.5384 | 2.6061 | 3.1119 | H6 | 2.8420 | 2.1881 | 1.1039 | 1.7829 | 1.7816 | | 2.5384 | 3.0960 | 3.1119 | 2.6061 | H7 | 2.0891 | 1.1052 | 2.1718 | 2.5210 | 3.0960 | 2.5384 | | 1.7636 | 2.9399 | 2.4041 | H8 | 2.0891 | 1.1052 | 2.1718 | 2.5210 | 2.5384 | 3.0960 | 1.7636 | | 2.4041 | 2.9399 | H9 | 1.0258 | 2.0426 | 2.7352 | 3.7413 | 2.6061 | 3.1119 | 2.9399 | 2.4041 | | 1.6235 | H10 | 1.0258 | 2.0426 | 2.7352 | 3.7413 | 3.1119 | 2.6061 | 2.4041 | 2.9399 | 1.6235 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| N1 |
C2 |
C3 |
116.120 |
|
N1 |
C2 |
H7 |
107.591 |
| N1 |
C2 |
H8 |
107.591 |
|
C2 |
N1 |
H9 |
108.547 |
| C2 |
N1 |
H10 |
108.547 |
|
C2 |
C3 |
H4 |
111.702 |
| C2 |
C3 |
H5 |
110.946 |
|
C2 |
C3 |
H6 |
110.946 |
| C3 |
C2 |
H7 |
109.592 |
|
C3 |
C2 |
H8 |
109.592 |
| H4 |
C3 |
H5 |
107.733 |
|
H4 |
C3 |
H6 |
107.733 |
| H5 |
C3 |
H6 |
107.604 |
|
H7 |
C2 |
H8 |
105.849 |
| H9 |
N1 |
H10 |
104.627 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBEPBE/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.494 |
|
|
|
| 2 |
C |
-0.144 |
|
|
|
| 3 |
C |
-0.403 |
|
|
|
| 4 |
H |
0.122 |
|
|
|
| 5 |
H |
0.120 |
|
|
|
| 6 |
H |
0.120 |
|
|
|
| 7 |
H |
0.116 |
|
|
|
| 8 |
H |
0.116 |
|
|
|
| 9 |
H |
0.224 |
|
|
|
| 10 |
H |
0.224 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.835 |
-0.939 |
0.000 |
1.256 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-23.519 |
2.367 |
0.000 |
| y |
2.367 |
-20.035 |
0.000 |
| z |
0.000 |
0.000 |
-19.027 |
|
| Traceless |
| | x | y | z |
| x |
-3.988 |
2.367 |
0.000 |
| y |
2.367 |
1.238 |
0.000 |
| z |
0.000 |
0.000 |
2.750 |
|
| Polar |
| 3z2-r2 | 5.500 |
| x2-y2 | -3.484 |
| xy | 2.367 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.172 |
0.202 |
0.000 |
| y |
0.202 |
4.618 |
0.000 |
| z |
0.000 |
0.000 |
4.562 |
<r2> (average value of r
2) Å
2
| <r2> |
0.000 |
| (<r2>)1/2 |
0.000 |
Jump to
S1C1
Energy calculated at PBEPBE/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -134.992427 |
| Energy at 298.15K | |
| Nuclear repulsion energy | |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Vibrational Frequencies calculated at PBEPBE/6-31G(2df,p)
Geometric Data calculated at PBEPBE/6-31G(2df,p)
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability